1 Bidirectional User Throughput Maximization Based on Feedback Reduction in LiFi Networks Mohammad Dehghani Soltani, Xiping Wu, Majid Safari, and Harald Haas Abstract Channel adaptive signalling, which is based on feedback, can result in almost any performance metric enhancement. Unlike the radio frequency (RF) channel, the optical wireless communications (OWCs) channel is fairly static. This feature enables a potential improvement of the bidirectional user throughput by reducing the amount of feedback. Light-Fidelity (LiFi) is a subset of OWCs, and it is a bidirectional, high-speed and fully networked wireless communication technology where visible light and infrared are used in downlink and uplink respectively. In this paper, two techniques for reducing the amount of feedback in LiFi cellular networks are proposed, i) Limited-content feedback (LCF) scheme based on reducing the content of feedback information and ii) Limited-frequency feedback (LFF) based on the update interval scheme that lets the receiver to transmit feedback information after some data frames transmission. Furthermore, based on the random waypoint (RWP) mobility model, the optimum update interval which provides maximum bidirectional user equipment (UE) throughput, has been derived. Results show that the proposed schemes can achieve better average overall throughput compared to the benchmark one-bit feedback and full-feedback mechanisms. I. I NTRODUCTION The ever increasing number of mobile-connected devices, along with monthly global data traffic which is expected to be 35 exabytes by 2020 [1], motivate both academia and industry to invest in alternative methods. These include mmWave, massive multiple-input multiple-output (MIMO), free space optical communication and Light-Fidelity (LiFi) for supporting future growing data traffic and next-generation high-speed wireless communication systems. Among these technol- This work has been submitted to IEEE Transactions on Communications. The authors are with the LiFi Research and Development Center, Institute for Digital Communications, The University of Edinburgh. (E-mail: [email protected]; [email protected]; [email protected]; [email protected]). July 14, 2018 DRAFT arXiv:1708.03324v1 [cs.IT] 10 Aug 2017
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1
Bidirectional User Throughput Maximization Basedon Feedback Reduction in LiFi Networks
Mohammad Dehghani Soltani, Xiping Wu, Majid Safari, and Harald Haas
Abstract
Channel adaptive signalling, which is based on feedback, can result in almost any performance
metric enhancement. Unlike the radio frequency (RF) channel, the optical wireless communications
(OWCs) channel is fairly static. This feature enables a potential improvement of the bidirectional user
throughput by reducing the amount of feedback. Light-Fidelity (LiFi) is a subset of OWCs, and it is
a bidirectional, high-speed and fully networked wireless communication technology where visible light
and infrared are used in downlink and uplink respectively. In this paper, two techniques for reducing
the amount of feedback in LiFi cellular networks are proposed, i) Limited-content feedback (LCF)
scheme based on reducing the content of feedback information and ii) Limited-frequency feedback
(LFF) based on the update interval scheme that lets the receiver to transmit feedback information after
some data frames transmission. Furthermore, based on the random waypoint (RWP) mobility model,
the optimum update interval which provides maximum bidirectional user equipment (UE) throughput,
has been derived. Results show that the proposed schemes can achieve better average overall throughput
compared to the benchmark one-bit feedback and full-feedback mechanisms.
I. INTRODUCTION
The ever increasing number of mobile-connected devices, along with monthly global data
traffic which is expected to be 35 exabytes by 2020 [1], motivate both academia and industry to
invest in alternative methods. These include mmWave, massive multiple-input multiple-output
(MIMO), free space optical communication and Light-Fidelity (LiFi) for supporting future growing
data traffic and next-generation high-speed wireless communication systems. Among these technol-
This work has been submitted to IEEE Transactions on Communications. The authors are with the LiFi Research and
Development Center, Institute for Digital Communications, The University of Edinburgh. (E-mail: [email protected];
Fig. 9: Transmitted overhead versus different number of subcarriers.
is higher for mobile UEs.
VI. CONCLUSION AND FUTURE WORKS
Two methods for reducing feedback cost were proposed in this paper: i) the limited-content
feedback (LCF) scheme, and ii) the limited-frequency feedback (LFF) method. The former is
based on reducing the content of feedback information by only sending the SINR of the first
subcarrier and estimating the SINR of other subcarriers at the AP. The latter is based on the
less frequent transmission of feedback information. The optimal update interval was derived,
which results in maximum expected sum-throughput of uplink and downlink. The Monte-Carlo
simulations confirmed the accuracy of analytical results. The effect of different parameters on
July 14, 2018 DRAFT
26
optimum update interval was studied. It was also shown that the proposed LCF and LFF schemes
provide better sum-throughput while transmitting lower amount of feedback compared to the
practical one-bit feedback method. The combination of the LCF with the update interval is the
topic of our future study.
APPENDIX
A. Proof of (25)
According to the RWP mobility model, the UE is initially located at P0 with the distance
r0 from cell center. The scheduler at the AP is supposed to allocate the resources to the UEs
as much as they require. Thus, the achievable data throughput of the UE at t = 0 is equal to
the requested data rate i.e., R(0) = Rreq. Hence, kreq can be obtained by solving the following
equation:
Rreq =Bd,n
K
kreq∑k=1
log2
Ge−4πkBd,nKw0
(h2 + r20)m+3
=Bd,n
K
kreq∑k=1
log2
(G
(h2 + r20)m+3
)+Bd,n
K
kreq∑k=1
log2
(e−4πkBd,nKw0
)
=kreqBd,n
Klog2
(G
(h2 + r20)m+3
)− 4π
w0
(Bd,n
K
)2
log2e
kreq∑k=1
k
=kreqBd,n
Klog2
(G
(h2 + r20)m+3
)− 2π
w0
(Bd,n
K
)2
(log2e)kreq(kreq + 1)
⇒ k2req+
1−log2
(G
(h2+r20)m+3
)2πBd,n
Kw0log2e
kreq+Rreq
2πw0
(Bd,n
K
)2log2e
=0.
(30)
The above equation is a quadratic equation and it has two roots where the acceptable kreq can
be obtained as follows:
kreq =
(log2
(G
(h2+r20)m+3
)2πBd,nKw0
log2e−1
)−
√√√√(1− log2
(G
(h2+r20)m+3
)2πBd,nKw0
log2e
)2
− 4Rreq
2πw0
(Bd,nK
)2log2e
2.
(31)
If Rreq � w0
8πlog2
(G
(h2+r20)m+3
), the approximate number of required subcarriers is kreq
∼=KRreq
Bd,n log2
(G
(h2+r20)m+3
) . With the parameters given in Table I, the constraint on the requested data
rate is Rreq << 350 Mbps.
DRAFT July 14, 2018
27
B. Proof of Proposition
The optimal solution of the OP given in (18) can be obtained by finding the roots of its
derivation that is ∂Er0,θ[T ]
∂tu= wu
∂Er0,θ[Ru]
∂tu+ wd
∂Er0,θ[Rd]
∂tu= 0. The expectation value of the
average downlink throughput is Er0,θ[Rd] =∫∫
r0,θRdfR0(r0)fΘ(θ)dθdr0 and its derivation is
equal to ∂Er0,θ[Rd]
∂tu= ∂
∂tu
∫∫r0,θ
RdfR0(r0)fΘ(θ)dθdr0. Since the function inside the integral
is derivative on the range (0, 2rc/v), the derivation operator can go inside the integral as∫∫r0,θ
∂Rd
∂tufR0(r0)fΘ(θ)dθdr0 [48], and this is the expectation value of the derivation of the
average downlink throughput, i.e., Er0,θ[∂Rd
∂tu]. Thus, we can conclude that ∂Er0,θ[Rd]
∂tu=Er0,θ[
∂Rd
∂tu].
Using the same methodology for uplink throughput we have ∂Er0,θ[Ru]
∂tu= Er0,θ[∂Ru
∂tu]. Then, the
derivation of (17) can be expressed as:
Er0,θ[∂T∂tu
]= wuEr0,θ
[∂Ru
∂tu
]+ wdEr0,θ
[∂Rd
∂tu
]. (32)
Hence, the root of Er0,θ[ ∂T∂tu ] = 0 will be the same as the root of ∂Er0,θ[T ]
∂tu= 0.
Using the Leibniz integral rule the derivation of (23) can be obtained as:
∂Ru
∂tu=−2(m+ 3)TuBu,n
Nt2u
(1−2tfb
tu
)(tu
2(m+ 3)log2
(Gu
(r2(tu) +h2)m+3
)+r0 cos θ
2vlog2
(r2(tu)+h2
)− (h2+r2
0 sin2θ)12
v ln(2)tan−1
(vtu − r0 cos θ
(h2+r20 sin2θ)
12
)− (h2+r2
0 sin2θ)12
v ln(2)tan−1
(r0 cos θ
(h2+r20 sin2θ)
12
)
−r0 cos θ
2vlog2
(r2
0 +h2)
+tu
ln(2)
)+TuBu,n
Ntu
(1−tfb
tu
)log2
(Gu
(r2(tu) +h2)m+3
)(33)
Using the sum of inverse tangents formula, tan−1(a) + tan−1(b) = tan−1(a+b1−ab
), (33) can be
further simplified as:
∂Ru
∂tu=−2(m+ 3)TuBu,n
Nt2u
(1−2tfb
tu
)(r0 cos θ
2vlog2
(r2(tu)+h2
r20 +h2
)
−(h2+r20 sin2θ)
12
v ln(2)tan−1
vtu
(h2+r20 sin2θ)
12
1− r0 cos θ(vtu− r0 cos θ)
h2 + r20 sin2θ
+tu
ln(2)
+TuBu,ntfbNtu
log2
(Gu
(r2(tu)+h2)m+3
).
(34)
This is the exact derivation of the average uplink achievable throughput respect to tu, however,
July 14, 2018 DRAFT
28
for vtu � h, this equation can be further simplified. Substituting r(tu) = (r20+v2t2u−2r0vtu cos θ+
h2)1/2 in logarithm term, ignoring the small terms and using the approximation ln(1 + x) ∼= x
for small values of x, we arrive log2
(1+v2t2u−2r0vtucosθ
r20+h2
)∼= log2
(1−2r0vtucosθ
r20+h2
)∼= −2r0vtucosθ
ln(2)(r20+h2).
Considering the rule of small-angle approximation for inverse tangent, it can also be approximated
by its first two terms of Taylor series as tan−1(x) ∼= x−x3/3 for small x. Noting that tfb � tu,
the approximate derivation is given as follows:
∂Ru
∂tu∼=−2(m+ 3)TuBu,n
ln(2)Nt2u
(1−2tfb
tu
)((vtu)3(h2+ r2
0 sin2θ)2
3v(h2 + r20)3
+ tu
−r20 cos2θtur2
0 +h2− tu(h2+r2
0 sin2θ)
h2 + r20
)+TuBu,ntfbNt2u
log2
(Gu
(r20 +h2)m+3
)= −2(m+ 3)TuBu,nv
2(h2 + r20 sin2θ)2tu
3N ln(2)(h2 + r20)3
+TuBu,ntfbNt2u
log2
(Gu
(r20 + h2)m+3
) (35)
Using the Leibniz integral rule to calculate the derivation of average downlink throughput, and
the sum of inverse tangents formula to simplify it, the derivation of average downlink throughput
is given as:
∂Rd
∂tu=−2(m+ 3)kreqBd,n
Kt2u
(r0cosθ
2vlog2
(r2(tu) + h2
r20 + h2
)+
tuln(2)
−(h2+r20 sin2θ)
12
v ln(2)tan−1
vtu
(h2 + r20 sin2 θ)
12
1− r0 cos θ(vtu−r0 cos θ)
(h2 + r20 sin2 θ)
.
(36)
This is the exact derivation of average downlink achievable throughput respect to tu, however,
using the approximation rules for vtu � h, the well-approximated derivation is given as follows:
∂Rd
∂tu∼=−2(m+ 3)kreqBd,n
Kt2u
(− r2
0 cos2 θtuln(2)(r2
0 + h2)− tu(h2 + r2
0 sin2 θ)
ln(2)(h2 + r20)
+(vtu)3(h2 + r2
0 sin2 θ)2
3v ln(2)(h2 + r20)3
+tu
ln(2)
)=−2(m+ 3)kreqBd,nv
2tu(h2 + r20 sin2 θ)2
3K ln(2)(h2 + r20)3
.
(37)
The exact optimum time, tu,opt, can be obtained numerically by solving (26) after substituting
∂Rd
∂tuand ∂Ru
∂tugiven in (33) and (36). However, we can approximately obtain a closed form
for optimum update interval denoted as tu,opt by using (35) and (37). Taking into account that
vtu � h the closed solution form for optimum update interval is given as:
DRAFT July 14, 2018
29
tu,opt∼=
( 3ln(2)2(m+3)
wutfbTuBu,nC1
wdv2NRreq + C2wuv2TuBu,n
)13
,
where
C1 =
Er0[log2
(Gu
(r20 + h2)m+3
)]Er0[log2
(G
(r20 + h2)m+3
)]Er0,θ
[(h2 + r2
0 sin2 θ)2
(h2 + r20)3
] , C2 = Er0[log2
(G
(r20 + h2)m+3
)].
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